Fun selects on those scale models! The viewing had me think: dhmartens may have solved the topic's deal: tote a scale model and do one of two things:
1. Actually hang glide the scale model and accept the super sink rate with real self pilot onboard.
2. Feed the scale model some unobtanium zap to grow the scale model to full size and have a great flight session. At the end of the session wipe the HG with shrinking moist and pack away the obtained scale model.
Nice go ...!





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AI ChatGPT wrote:In fiction, it is certainly possible to imagine a magical fluid or potion that could cause a scale model hang glider to grow into a full-sized hang glider. However, this would require suspending disbelief and accepting that such a fluid or potion exists within the rules of the fictional universe.
The exact details of how such a fluid or potion would work would depend on the specific rules and mechanics of the fictional universe. For example, the fluid could contain special growth agents that cause the materials of the scale model to rapidly expand and transform into a full-sized hang glider. Alternatively, the potion could contain magical energy that causes the materials of the scale model to transform into a full-sized hang glider through a more mystical process.
Ultimately, the mechanics of how the magic fluid or potion would work to transform the scale model hang glider into a full-sized hang glider would be up to the imagination of the author or creator of the fictional universe.
Maybe just get to the site with the toted scale model and shrink oneself and then pilot the deal. Finishing the session, expand self to normal again.
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AI ChatGPT wrote:Both 7075-T6 and 6061-T6 are popular aluminum alloys that are commonly used in aerospace and structural applications. However, they have slightly different mechanical properties that can affect their buckling behavior.
Assuming the 5 ft long, 2 inch outside diameter, and 1/32 inch wall thickness aluminum tube is perfectly straight and uniform, we can calculate the critical buckling load using the Euler buckling equation:
P = (π²EI)/(KL)
Where P is the critical buckling load, E is the modulus of elasticity, I is the area moment of inertia, K is the effective length factor, and L is the length of the column.
For both 7075-T6 and 6061-T6 aluminum tubes, we can calculate their respective critical buckling loads and compare them.
For 7075-T6 aluminum tube:
Modulus of elasticity (E) = 71.7 GPa
Area moment of inertia (I) = π/4 * (2 in)^4 - π/4 * (1.9375 in)^4 = 5.2 × 10^-4 m^4
Effective length factor (K) = 1 (assuming pinned-pinned boundary conditions)
Length (L) = 5 ft = 1.524 m
Plugging in these values into the Euler buckling equation, we get:
P = (π² * 71.7 GPa * 5.2 × 10^-4 m^4) / (1 * 1.524 m) = 34.3 kN
For 6061-T6 aluminum tube:
Modulus of elasticity (E) = 68.9 GPa
Area moment of inertia (I) = π/4 * (2 in)^4 - π/4 * (1.9375 in)^4 = 5.2 × 10^-4 m^4
Effective length factor (K) = 1 (assuming pinned-pinned boundary conditions)
Length (L) = 5 ft = 1.524 m
Plugging in these values into the Euler buckling equation, we get:
P = (π² * 68.9 GPa * 5.2 × 10^-4 m^4) / (1 * 1.524 m) = 33.0 kN
Comparing the critical buckling loads of the two aluminum tubes, we see that the 7075-T6 aluminum tube has a slightly higher critical buckling load than the 6061-T6 aluminum tube. This is due to the higher modulus of elasticity of 7075-T6 aluminum, which means it can withstand higher stresses before buckling. However, the difference in critical buckling load is relatively small, and both tubes should be able to withstand similar loads before buckling occurs. It is worth noting that these calculations assume ideal conditions and do not account for imperfections or variations in the material properties that can affect the buckling behavior of the aluminum tubes.
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Misc. notes toward thread's topic:
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How lines that cause compression in a beam attach to the end of the beam in compression can significantly affect the buckling behavior of the compressed beam.
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https://books.google.com/books?id=ljSn7 ... ns&f=false